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The Late Cambrian to Neogene Evolution of the Khanom Core Complex (Peninsular Thailand) 卡农岩心群(泰国半岛)晚寒武世至新近纪的演变
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-01-12 DOI: 10.2113/2024/lithosphere_2023_272
Urs S. Klötzli, Bernhard Neugschwentner, Jolanta Burda, Pitsanupong Kanjanapayont, Qiu-Li Li, Yu Liu, Patrik Konečný, Punya Charusiri
The Khanom Core Complex in Peninsular Thailand is a part of the crystalline basement of Sundaland and plays a key role in our understanding of the evolution of Thailand and SE Asia. The complex comprises ortho- and paragneisses, schists, meta-volcanics, subordinate calcsilicate rocks, and postkinematic granitoids. New petrochronological data reveal that the sedimentation and metamorphism of the paragneiss precursors (Haad Nai Phlao complex, Khao Yoi paragneisses) occurred in the Late Cambrian at the latest. A syn- to postsedimentary andesitic intrusion/extrusion in the Haad Nai Phlao complex at 495 ± 10 Ma defines a minimum age for the former event(s). In the Early Ordovician (477 ± 7 Ma), the Haad Nai Phlao complex and the Khao Yoi paragneisses were intruded by the Khao Dat Fa granite. During the Indosinian orogenic events, the Laem Thong Yang (211 ± 2 Ma) and Haad Nai Phlao (210 ± 2 Ma) granitoid plutons were intruded. Immediately afterward (ca. 208–205 Ma), the first metamorphic overprinting of the Laem Thong Yang granite and the Haad Nai Phlao complex including the Khao Dat Fa granite occurred. A second metamorphic overprinting of all lithological units and the contemporaneous intrusion of the Khao Pret granite followed in the Late Cretaceous and Early Paleogene (ca. 80–68 Ma). The tectonic formation of the core complex took place in the Eocene (<42 Ma), followed by exhumation and regional cooling below ca. 450°C and the latest cooling to ca. 120°C in the Miocene (ca. 20 Ma). The evolutionary data show that the Khanom Core Complex is part of Sibumasu, and its Late Cretaceous-Neogene cooling pattern and exhumation history can be directly related to the northward drift of India.Thailand is located on the geological entity known as Sundaland, which consists of Gondwana-derived continental terranes that accreted over time to build the present-day mainland of Indochina [1, 2]. Two main continental terranes can be distinguished, Sibumasu in the west and Indochina in the east, along with an interjacent arc, called Sukhothai. Both terranes are crucial to understand the geological evolution of Gondwana, the various Tethys oceanic domains, Sundaland, and Southeast Asia. However, there is no agreement on the nature and exact locations of their boundaries, the characteristics of the basement evolution, or the tectonic models of their amalgamation (References [2-5] and references therein). This problem is accentuated by the scarcity of crystalline basement exposures. The available basement data are limited to three regions of exposure in northern and southeast Thailand and on the Thai peninsula.The first description of crystalline basement rocks in Thailand was published by Heim and Hirschi [6]. These rocks are typically high- to medium-temperature low-pressure metamorphic and intermediate to acidic plutonic rocks [1, 7, 8]. Often, they are overlain by fossiliferous Phanerozoic sediments [1, 9]. Consequently, the first to assign a Precambrian age to the g
泰国半岛的卡诺姆岩芯复合体是巽他兰结晶基底的一部分,对我们了解泰国和东南亚的演化起着关键作用。该岩群由正长岩和副片麻岩、片岩、元火山岩、次生钙硅酸盐岩和后生花岗岩组成。新的岩石年代学数据显示,副片麻岩前身(Haad Nai Phlao 复合岩、Khao Yoi 副片麻岩)的沉积和变质作用最晚发生在晚寒武纪。Haad Nai Phlao岩群在495±10Ma时发生了一次同沉积至后沉积安山岩侵入/挤出作用,从而确定了前一事件的最低年龄。在早奥陶世(477±7Ma),Haad Nai Phlao岩群和Khao Yoi副片麻岩被Khao Dat Fa花岗岩侵入。在印支期造山运动中,Laem Thong Yang(211 ± 2 Ma)和 Haad Nai Phlao(210 ± 2 Ma)花岗岩岩体侵入。紧接着(约 208-205 Ma),Laem Thong Yang 花岗岩和 Haad Nai Phlao 复合岩(包括 Khao Dat Fa 花岗岩)发生了第一次变质叠压。随后,在晚白垩世和早古新世(约 80-68 Ma),所有岩性单元发生了第二次变质叠压,并同时侵入了 Khao Pret 花岗岩。岩芯复合体的构造形成发生在始新世(10 至 ~40 云母晶体,大小约为 1-2 毫米)。为了与已发表的描述保持一致,所调查的样品按照 Kosuwan [16]的命名方案和岩相图谱进行分类。调查样品为:LTY片麻岩(TH1608,KN30:09°5'19.8 "N/099°54'36.12 "E;TH1610:09°5'26.1 "N/099°53'38.1 "E;KN71:09°6'31.98 "N/099°54'5.90 "E)。HNP-a 片麻岩(TH1611:09°8'22.7 "N/099°52'33.4 "E).细粒 HNP 片麻岩(KN19:09°8'22.7 "N/099°52'33.4 "E).粗粒 HNP(HNP-cg)片麻岩(TH1612,KN68:09°8'21.1 "N/099°52'35.9 "E; KN18: 09°8'11.25 "N/099°50'24.04 "E; KN54: 09°7'56.40 "N/099°50'26.06 "E).Tong Yi leucocratic gneiss (TH1613: 09°6'49.9 "N/099°53'55.3 "E).Khao Pret granite (KN21: 09°6'43.28 "N/099°52'15.79 "E).LTY片麻岩(TH1608,KN30:09°5'19.8 "N/099°54'36.12 "E;TH1610:09°5'26.1 "N/099°53'38.1 "E;KN71:09°6'31.98 "N/099°54'5.90 "E).HNP-a片麻岩(TH1611:09°8'22.7 "N/099°52'33.4 "E).细粒 HNP 片麻岩(KN19:09°8'22.7 "N/099°52'33.4 "E).粗粒 HNP(HNP-cg)片麻岩(TH1612,KN68:09°8'21.1 "N/099°52'35.9 "E;KN18:09°8'11.25 "N/099°50'24.04 "E; KN54: 09°7'56.40 "N/099°50'26.06 "E).Tong Yi leucocratic gneiss (TH1613: 09°6'49.9 "N/099°53'55.3 "E).Khao Pret granite (KN21: 09°6'43.不同岩性的实地照片见图 3,薄片照片见图 4。LTY 是一种一般为粗粒、部分略带酸蚀作用的龙纹片麻岩,产于 KCC 东南部的 Thong Yi 海滩、Hin Lat 瀑布、Khao Phlai Dam 和 Phlai Dam 海滩(图 2)。LTY 的平均矿物组合为 K 长石(40-50 Vol%,Or = 90)、石英(25-30 Vol%)、斜长石(15-20 Vol%,An = 15-30)和斜长石(5-10 Vol%;图 3(a),3(e))。斑岩纹理主要由 K 长石和稀疏的斜长石螺旋岩组成,两者的大小都不超过几厘米。基质由细粒石英、斜长石和斜长石组成,其中斜长石颗粒的取向决定了褶皱。除了一些大的钾长石碎块和斜长石外,矿物颗粒都是正方体。钾长石经常出现卡尔斯巴德孪晶和微斜长石孪晶、透辉石解理以及沿晶体边缘的前安山岩熔体残余(图 4(b))。在 K 长石中存在大小不一的石英、斜长石、斜长石、磷灰石、独居石和锆石包裹体。斜长石的特征是多合成孪晶、残余岩浆分带以及局部强烈的绢云母蚀变。在K长石和斜长石的接触面上,有时会出现取代K长石的麦饭石。石英颗粒表现出动态再结晶、晶界迁移,在某些地方还表现出微弱的形状偏好取向。黑云母大多沿着长石螺旋线排列,形成特征性的团块,并在锆石和独居石包裹体周围显示出扭结带和褶彩晕。次要成分有白云母、绿泥石、闪石、黝帘石、绢云母、钛铁矿,在某些地方还有电气石。附属成分有锆石、独居石和氙石(通常会形成特有的副成因)、磷灰石和铁氧化物。大部分的锆石和独居石都与黑云母团块伴生。在KCC中部和东北部的Nai Phlao海滩和Samet Chun瀑布周围,可以发现HNP的外围地区(图2)。它由两个品种组成,即粗粒和细粒生物片麻岩。这两个岩种之间的结构、纹理和年代关系尚不确定。一方面,它们交替出现。 加权平均年龄为 41.9 ± 6.5 Ma。加权平均年龄为 41.9 ± 6.5 Ma.,KN19-1号斜长石样品的总融合 39Ar/40Ar 年龄为 23.8 ± 8.8 Ma (40Ar/36Ar = 246 ± 119),五个斜长石馏分的总融合年龄介于 29.6 ± 12.4 (KN21-6b; 40Ar/36Ar = 497 ± 411) 和 46.2 ± 7.5 Ma 之间。五种斜长石馏分的总融合年龄分别在 29.6 ± 12.4 (KN21-6b; 40Ar/36Ar = 497 ± 411) 和 46.2 ± 7.5 Ma (KN21-1b; 40Ar/36Ar = 1325 ± 991) 之间,40Ar/36Ar 和 39Ar/40Ar 之间没有系统关系。所有五个生物岩馏分的加权平均 39Ar/40Ar 年龄为 40.7 ± 1.4。对 KN21-1 样品进行了五步加热实验。每一步的 39Ar/40Ar 年龄在 38.2 ± 2.5 至 41.9 ± 2.3 Ma 之间。除第一个低温步骤外,40Ar/36Ar 比率均≥ 1994 ± 1612。分步加热实验的加权平均 39Ar/40Ar 年龄为 40.7 ± 1.4 Ma。两个黝帘石馏分(KN21-1 和 KN21-6)的 39Ar/40Ar 年龄分别为 39.8 ± 3.7 Ma(40Ar/36Ar = 782 ± 51)和 34.3 ± 3.8 Ma(40Ar/36Ar = 363 ± 38)。加权平均年龄为 37.1 ± 5.2 Ma。从岩相学上看,LTY 是一种均质粗粒生物橄榄岩,可解释为变质火成岩体。与 Kosuwan [16]提供的地球化学数据相比
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Numerical Study on Characteristics of Stick-Slip Instability of Coal-Rock Parting-Coal Structure under Lateral Unloading 侧向卸荷下煤岩分煤结构粘滑失稳特性的数值研究
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-01-12 DOI: 10.2113/2024/lithosphere_2023_172
Heng Zhang, Guang-Jian Liu, Xian-Jun Ji, Wen-Hao Cao, Ya-Wei Zhu, Sher Bacha
Unloading excavation can increase the possibility of rock burst, especially for coal seam with rock parting. In order to explore the evolution process of rock burst under lateral unloading, the combination of in situ measures and numerical experiments is used to study. The following four points were addressed: (1) the coal seam with rock parting easily causes the stick-slip and instability along the interface, and the process of stick-slip and instability has hysteresis characteristics; (2) the greater the degree of unloading or the smaller the interface friction angle of the Coal-Rock Parting-Coal Structure (CRCS), the more likely it is for stick-slip and instability to occur; (3) the abnormal increase of shear stress and slip dissipation energy can be used as the precursory information of the stick-slip and instability of CRCS; (4) the damage intensity of rock burst induced by stick-slip and instability of CRCS can be reduced by reducing the unloading speed or increasing the roughness of interface. The research results can be used for early warning and controlling of dynamic disaster induced by stick-slip instability in coal seam with rock parking.The slip-staggered rock burst is caused by the slip dislocation of the internal related structure, which mainly occurs in the fault, coal seam separation, and abnormal change area of coal seam dip angle. The coal seam separation is a typical occurrence structure in coal mines of China, which causes the transformation of coal and rock structures, and commonly the Coal-Rock Parting-Coal Structure (CRCS) is formed by rock parting upper and lower coal seams [1, 2]. The natural CRCS is in a stable triaxial stress state. The process of roadway excavation can cause the redistribution of surrounding rock stress and cause the horizontal stress to be gradually released, and the CRCS also changes from a three-dimensional stress state to a lateral unloading state [3-6]. As the interface of coal and rock parting is weak, the process of lateral unloading may cause stick-slip and instability along the weak surface, which easily leads to rock burst accidents.In recent years, with the rapid development of science and technology, the research methods of rock mechanics are gradually enriched. The deformation and failure mechanism of unloading coal/rock mass is gradually revealed, and the mechanism of stick-slip instability of the contact surface is also constantly verified [7]. Such as He et al. [8-10] designed a true-triaxial rock burst test simulation system and simulated the lateral sudden unloading process caused by deep rock excavation. Lu et al. [11] studied the precursory characteristics of rock burst induced by fault stick-slip instability through field observations and biaxial direct shear friction experiments and explained the influence of friction coefficient on stick-slip instability. Liu et al. [12] confirmed that the rock parting structure also has the characteristics of stick-slip and instability under th
基于此,本文以云和煤矿(YCM)C5301工作面为研究背景,以煤层带岩停车驱动诱发结构滑动为研究对象,采用UDEC数值模拟技术研究了CRCS的粘滑失稳过程,研究了卸载速度和节理粗糙度系数(JRC)对复合结构粘滑失稳的影响,提出了横向卸载诱发粘滑失稳冲击灾害的防治措施。永利国际娱乐平台位于中国山东省济宁市。图 1 是 C5301 长壁工作面的平面布置图。C5301长壁工作面标高为-600米至-684米,平均标高为-642米;开采3#煤层厚度为5.4米至10.3米,平均厚度为8.1米;倾角为9°至20°,平均倾角为14°。表 1 列出了长壁工作面煤层和岩层的岩性。C5301 长壁工作面煤层中存在岩层破碎带(见图 1)。微震(MS)是一种利用岩石断裂产生的波浪效应进行定位的监测方法,在煤矿和隧道工程中应用广泛[18,19]。YCM 安装了 KJ648 MS 系统和 19 个检波器。该系统可完成实时监测、数据处理和震源三维可视化等功能。基于微地震到达时差和到达时差商的原理[20]。在 C5301 长壁工作面周围(如图 1 所示)共布置了四个检波器,分别命名为 C5301p1、C5301p2、C5301g1 和 C5301g2。2018年12月10日至2019年1月10日,C5301长壁工作面推进距离为116米,在巷道掘进过程中,分岩区经常发生大能量MS事件,这可能与CRCS的粘滑失稳有关。事件计数和峰值能量都呈现出明显的 "积累-释放-积累 "循环。Lu 等人[21]指出,断层粘滑失稳过程中存在明显的振动突变,是典型的能量积累过程。这与分岩区开挖引起的振动变化特征是一致的。据观察,当能量积累到滑移条件时,将沿 CRCS 的界面发生滑移和失稳过程。同时,由于界面的不规则性,在滑移和失稳过程中,摩擦系数会随着界面粗糙度的变化而逐渐变化。因此,CRCS 的滑移和失稳过程呈现出 "滑移-稳定-滑移 "现象,这与断层粘滑失稳是一致的。在C5301迎头掘进初期,震源主要集中在分岩厚度明显变化的区域。2018年12月22日,定位到一个能量为3.39×105 J(>105 J)的MS事件,定义为矿井强震,称之为矿井强震(SME)。通过分析,其成因是初期掘进扰动,导致-725北头面进尺CRCS发生粘滑失稳。随着巷道推进至分岩区域,岩源逐渐向巷道两侧及后方转移。2018年12月26日至2019年1月10日,发生了三次能量较大的MS事件,能量分别为1.70×105、1.20×105和1.43×105 J,其中两次位于巷道附近。研究证明,巷道开挖诱发的 CRCS 粘滑失稳具有明显的滞后特征,随着深部岩体的开挖,水平应力呈阶梯式递减趋势[22]。根据 C5301 长壁工作面分岩的发生特征,建立了横向卸载下 CRCS 粘滑失稳的力学模型。其中,σθ为法向应力,σ3和σ′3为水平应力,τ1和τθ为剪应力,l和h为模型宽度和高度,θ为界面角。 假设煤块和岩块都是刚性的,且岩块没有损坏,那么当横向卸载使水平应力逐渐减小时,其中 N 和 Δδ 分别为卸载步距和卸载坡度。因此,如果此时 A 为固定值,则在横向卸荷作用下水平应力会逐渐减小。因此,CRCS 的滑移和不稳定性与横向卸载下的卸载步长和卸载梯度密切相关。卸载步长越长,卸载梯度越大,CRCS 就越容易滑移。将方程(7)代入方程(4):IfThen由此可见,f(φ) 是一个单调递增函数。因此,摩擦角越大,CRCS 越稳定。粘滑是指界面的剪应力在滑动过程中不断增大和急剧减小的滑动过程,而稳滑是指接触面的剪应力基本稳定的滑动过程[23]。图 5 显示了粘滑失稳的过程,分为初始闭塞、上坡、下坡和再闭塞四个过程。在上坡滑动过程中,法向应力(σ)起负作用,否则σ起正作用。根据耶格尔摩擦定律:其中,τ1 和 τʹ1 分别为界面在上坡和下坡时的剪应力,τmax 和 τmax ʹ 分别为界面在上坡和下坡时的最大剪应力,μ 和 σ 分别为界面的摩擦系数和法向应力,c 为界面的内聚力,Δτ 为界面在上坡和下坡时的剪应力波动值。假设两侧坡角一致,且块体未发生破裂,则剪应力将随界面的上坡和下坡而波动,剪应力波动值为Δτ=2μσ。同时,当侧向卸荷产生的水平应力F恒定时,界面的滑移速度会随着剪应力的变化而波动,这也是产生粘滑的原因。根据现场勘测和分岩结构力学分析,建立了 UDEC 数值模型来研究侧向卸荷引起的 CRCS 粘滑和失稳,数值模型如图 6 所示。模型的宽度和高度分别为 50 毫米和 100 毫米,上下设置两块刚性加载板。底部加载板固定,顶部加载板保持轴向恒载 σ1,初始约束压力设为 σ3。采用侧向卸载法模拟巷道开挖后水平应力的缓慢卸载过程,力卸载速度单位为 Pa/步。在 UDEC 离散单元中,岩石被认为是由岩块和节理面组成的结构。岩块和节理有各自的微参数。这些微参数无法通过实验室力学试验直接获得,因此需要在模拟前进行反演校准[24, 25]。参数标定过程如下:首先,通过单轴压缩实验获得煤和岩石分块的变形模量(E)和泊松比(μ)。根据国际岩石力学学会(ISRM)的规定,单轴压缩校核试验采用直径为 50 mm、高度为 100 m 的煤岩裂隙样品,数值模型与校核样品尺寸一致[26]。图 7 显示了单轴压缩下煤块和岩块样品的数值结果和实验结果。数值模型中的块体体积模量(K)和剪切模量(G)可通过以下公式(13)和公式(14)计算得出[27]。表 3 显示了校准后煤块和岩块的微观参数。接缝的法向刚度 kn 和剪切刚度 ks 由公式 (15) 和公式 (16) [27] 得出。表 4 显示了校准后的接缝法向刚度和剪切刚度。其中,ΔΖmin 是垂直方向上接触邻接区的最小宽度。巴西圆盘使用了直径为 50 毫米、厚度为 25 毫米的圆盘试样,数值模型与校准试样尺寸一致[28]。图 8 显示了巴西圆盘测试下煤和岩石分型样本的数值和实验结果。 其中,nc 为接触点个数,fs 和 fʹs 分别为接触点当前和之前的剪切力,us 为一个时间步长内剪切位移的增量;Ukw 通过求和各网格点的动能来计算[27]。在初始卸载阶段,Ujf 和 Uk 的值相对较小,并随着卸载时间的增加而逐渐增大,且两者与整体变化具有较强的耦合性。在粘滑前兆阶段,Ujf 很快达到高值,然后基本保持稳定,而 Uk 值始终在 0 左右,这表明 Ujf 对粘滑和不稳定的响应早于 Uk。在粘滑和失稳阶段,耗散能量迅速增加,能量 Ujf 的峰值随 CRCS 的粘滑和失稳而波动,但动能逐渐增加。总的来说,侧向卸载会诱发 CRCS 的粘滑和失稳。通过对粘滑和失稳特征的分析可以发现,剪应力的异常增大可以作为 CRCS 粘滑和失稳的前兆信息,剪应力的峰值点可以作为粘滑和失稳的起点。根据裂缝发展特征的分析,煤的失稳表现为断裂,岩石分层的失稳表现为滑移。根据耗能特性分析,滑移耗能对粘滑和失稳的响应早于动能,滑移耗能的异常增加也可作为粘滑和失稳的前兆。随着粘滑的发生,CRCS 的动能逐渐增大,这也是滑移诱发岩爆发生的直接原因。巷道掘进速度不同,围岩体的应力卸荷速度也不同。一般来说,掘进速度越快,应力卸载速度也越快。为了研究卸载速度对 CRCS 粘滑和失稳的影响,我们对不同卸载速
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Study of the Effect of Drying and Wetting Cycles and Water Content on the Shear Characteristics of Tailing Sands 干燥和润湿循环及含水量对尾砂剪切特性的影响研究
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-01-12 DOI: 10.2113/2024/lithosphere_2023_320
Yakun Tian, Zhijun Zhang, Min Wang, Lingling Wu, Lin Hu, Rong Gui
The mechanical characteristics of tailing sands have an important impact on the safety and stability of the tailing dams. Fully understanding the effect of drying and wetting cycles (DWC) and water content on the characteristics of tailing sands is urgently needed. In this study, direct shear tests were first carried out to analyze the effect of DWC and water content on the macroscopic mechanical characteristics of tailing sands. Then, the mesoscopic mechanical behavior of tailing sands with different water contents under the action of DWC was studied by using PFC2D particle flow software. The results showed that the effect of DWC on the shear properties of tailing sands is more pronounced than water content. The cohesive force and the internal friction angle increase first and then decrease with the increasing water content. With the increasing number of DWC, the cohesive force and the internal friction angle all decreased to varying degrees. The results of the mesoscopic mechanical analysis indicated that after experiencing the DWC, the force chain of the sample gradually thickens to form a coarse force chain network area, and the number of cracks inside the sample is significantly larger than that of the sample that has not experienced the DWC. The results of this study are of great significance for understanding the macroscopic and mesoscopic shear failure mechanism of tailing sands under the effects of DWCs and water content.The tailing dam is a man-made debris flow hazard with high potential energy, and there are many unstable factors in its operation process. The collapse of the tailing dam not only affects the production of mining enterprises but also brings huge disasters to the inhabitants. Due to periodic changes in water conditions (i.e., rainfall infiltration, water evaporation, and repeated elevation and decline of the infiltration line), the tailing dam is subjected to long-term drying and wetting cycles (DWCs) during operation. It was found that the DWCs will lead to a decrease in the mechanical properties of the soil, and the changes in water content also affect the microstructure and mechanical properties of the soil. Under the action of DWC and water content, the matric suction and shear strength of the soil will change, thus affecting the stability of the soil structure. Therefore, a comprehensive understanding of the influence of the DWC and water content on the characteristics of tailing sands is of great significance for the long-term safety and stability of the tailing dam.A substantial effort has been made on the changes in the physical properties and mechanical behavior of rock materials under the action of cyclic wetting and drying [1-21]. The properties of rock materials (i.e., porosity, longitudinal wave velocity, compressive strength, shear strength, etc.) are significantly influenced by DWCs. Zhou et al. [7] studied the dynamic tensile strength characteristics of rocks after cyclic drying and wetting. They inferred
土壤的粒径及其成分对力学性能起着决定性作用。粒度一般以级配为特征。在本次试验所取的尾矿砂样品中,90% 以上的颗粒粒径大于 0.075 毫米,因此选择筛分法进行颗粒分析试验。取 8 个 400 克尾矿砂样品进行平行筛分试验,得到的粒度分布累积曲线如图 2 所示。样品的颗粒级配参数见表 2。可以看出,不均匀系数(Cu)为 1.37,曲率系数(Cc)为 1.04,不符合 Cu ≥ 5 和 Cc = 1-3 的要求。为了完全去除尾砂中的水分,收集的尾砂在温度为 120°C 的烘箱中烘干,直到质量不再发生变化。根据尾矿砂的自然含水量和最佳含水量,在干燥后的尾矿砂中加水,制备不同含水量(10%、12%、14%、16% 和 18%)的样品。然后将制备好的尾砂装在密封袋中,放置 24 小时,使其与水充分融合。为充分模拟现场的 DWCs,在 DWCs 之前,将尾砂样分三层压实到尺寸为 Φ61.8 mm × 20 mm 的环刀中。环刀的底部用阻砂透水土工布包裹,并用扎线带固定,环刀的上部用滤纸和保鲜膜覆盖,以防止水分流失。首先,在铁箱底部铺上一层准备好的尾矿砂,尺寸为 188 mm × 138 mm × 38 mm,并压实。然后,将环刀试样放在第二层上,同时用尾砂填满空隙。最后,在环刀试样上方填满尾砂,并再次压实。密封铁箱,静置 72 小时。这种方法不仅能有效避免在 DWCs 过程中添加水对样品表面的干扰,还能消除取样过程中人为因素的干扰。图 4 所示为循环干燥湿润装置。在前期试验中发现,经过 5 次 DWC 后,尾矿砂的力学性能趋于稳定,并呈现出一定的规律性。在本研究中,不同含水率的样品分别经历了 1、2、3、4 和 5 次 DWCs。同时还设置了一组未经历 DWC 的对照试验。每组有 3 次平行测试,测试结果为 3 次测试的平均值。通过低温干燥和人工浇水模拟自然环境中的 DWC 过程。根据现场的自然环境,确定 DWC 过程中含水量的变化范围控制在 3% 至 23% 之间。DWC 过程如图 5 所示(以含水率 16% 为例)。请注意,样品安装完毕后,要使用含水量相同的湿棉花围住容器。加载顺序设定为 50、100 和 200 kPa。为避免试验过程中含水量的变化,剪切速率选择为 0.8 毫米/分钟,并采用固结快速剪切法。直接剪切试验过程如图 6 所示。在垂直荷载为 50、100 和 200 kPa 的条件下,得到了不同含水率的尾矿砂在 DWCs 条件下的剪应力和位移关系曲线。由于篇幅有限,仅列出经历 0 DWCs 和 5 DWCs 的尾矿砂的剪应力和位移关系曲线(图 7)。从图中可以看出,尾砂的剪应力和位移关系曲线可分为三个阶段:弹性阶段、峰值阶段和稳定阶段。在弹性阶段,随着垂直荷载的增加,剪应力与位移的关系曲线变得更陡,表明尾砂的初始剪切模量与施加的垂直荷载呈正相关。在峰值阶段,剪应力达到最大值,此时颗粒间的粘结力达到最大。在稳定阶段,随着位移的增加,剪应力不再有很大的变化,甚至呈下降趋势,这表明样品已达到剪切强度。此时,试样已被破坏,也可称为破坏阶段。 在相同含水量和相同垂直荷载条件下,经过 5 次循环干燥和湿润后,尾矿砂的剪切强度下降,与剪切强度相对应的剪切位移变小。这表明循环干燥和湿润改变了尾矿砂的力学性能,缩短了弹性变形阶段。上述现象是由于在 DWC 过程中,水分的蒸发和积累改变了样品原有的孔隙结构。实验还发现,样品在循环干燥和润湿后体积略有膨胀。在 DWCs 的作用下,样品内部的孔隙增大,原来的颗粒胶结物被分离成分散的颗粒。样品的强度由孔隙间结合的水和颗粒来维持。在直接剪切试验中,脆性颗粒的强度较低,因此在相同的垂直荷载作用下,试样更容易被破坏。在大多数情况下,含水量为 16% 的样品的剪切强度高于其他含水量的样品。从剪切应力和位移关系曲线可以看出,循环干湿和含水量对尾矿砂的剪切强度都有影响。为了进一步分析干湿度和含水量对尾矿砂剪切特性的影响,有必要研究尾矿砂内聚力和内摩擦角的变化规律。以法向应力δ为横轴,剪切应力τ为纵轴,通过库仑定律拟合剪切强度曲线数据,得到内聚力和内摩擦角。尾矿砂在含水率和 DWCs 作用下的内聚力变化特征如图 8 所示。可以看出,在天然含水量下,尾矿砂的内聚力并没有达到最大值。它随着含水量的增加先增大后减小。这与许多学者的结论一致[34-36]。造成这种现象的主要原因是天然含水量的尾矿砂样品相对干燥,颗粒间的水分子数量较少。颗粒之间的牵引力较弱,无法使尾矿颗粒牢固地粘结在一起。随着含水量的增加,水分子数量增加,颗粒之间形成液桥力,从而产生更大的内聚力。先前的研究[35]表明,随着含水量的增加,母吸力也会减小。含水量达到 12% 后,因垫吸力下降而导致的胶结减弱程度大于因液桥力而导致的胶结增强程度。当含水率超过 12% 时,尾矿砂的粘聚力呈下降趋势。在相同含水率条件下,尾矿砂的粘聚力在 DWCs 后都有不同程度的下降。在相同含水率条件下,尾矿砂在经过一次循环干燥和湿润后,内聚力都有不同程度的下降,而且随着循环干燥和湿润次数的增加,内聚力的下降趋势越来越平缓。在 DWC 过程中,尾矿砂内部孔隙结构变得疏松,粘结水膜厚度减小,导致内聚力下降。从图 9 中可以看出,随着含水量的增加,尾砂的内摩擦角先增大后减小。它在最佳含水量(16%)时达到最大值。在含水量达到 16% 之前,由于液桥力的存在,摩擦强度增强,从而增加了颗粒之间的牵引力。当含水量增加到一定程度时,水膜会变厚,从而减弱尾砂颗粒之间的接触。 水对颗粒表面的润滑作用使颗粒之间的连接容易断裂,导致颗粒之间的摩擦强度降低。内摩擦角随着 DWCs 数量的增加而逐渐减小。这是由于循环干燥和润湿后尾矿砂样品的孔隙结构发生了变化。DWCs 使颗粒之间的距离变大,从而导致摩擦强度降低。此外,样品内部的水分一直在变化,作为润滑剂的水也会对颗粒之间的相互摩擦产生影响。在 PFC 理论中,土壤或岩石材料被模拟为具有法向和切向刚度的圆形或球形颗粒的集合。每个颗粒都通过粘合剂与相邻颗粒接触。PFC 有两种不同的接触模型,即接触结合模型和平行结合模型 [37-39]。在接触结合模型中,粒子之间的接触可以想象成一对具有法向和切向刚度的弹簧,可以在接触点传递弹性相互作用力,但不能抵抗粒子的旋转和拉伸。在平行结合模型中,颗粒间的接触可想象为一组均匀分布在矩形截面上的弹簧,以接触面上的接触点为中心。它不仅能传递颗粒间的弹性相互作用力,还能抵抗旋转产生的力矩。在接触结合模型中,只要颗粒保持接触,结合就会断开,接触刚度就会保持有效。然而,在平行键模型中,键的断裂会导致刚度下降。平行粘结模型能更好地反映土壤或岩石材料的实际属性。因此,我们在研究中采用了平行粘结模型。图 10 显示了平行粘结模型在 PFC2D 中的构成行为。尾砂的颗粒半径集中在 0.125-0.15 mm 范围内,粒径相对较细。直接剪切试样的尺寸为 Φ61.8 × 20 mm。在建立 PFC 模型的过程中,如果采用真实的粒度和级配,会导致颗粒数量较多,对计算机配置要求较高。为了方便建模和提高计算效率,模型中的颗粒半径只需满足宏观力学性能即可。许多学者研究了尺寸效应对数值模拟的影响。Liu 和 C
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引用次数: 0
Continental Arc Accumulation Mafic Rocks in the Mid-Upper Crust: Constraints From the Early Eocene Hornblende Gabbro–Diorite in the Tengchong Block, Southeastern Extension of Tibet 中上地壳大陆弧堆积岩浆岩:西藏东南延伸腾冲地块早始新世角闪长辉长岩-闪长岩的制约因素
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-01-12 DOI: 10.2113/2024/lithosphere_2023_319
Tai Wen, Shao-wei Zhao, Xiao-yu Fang, Xian-Zhi Pei, Zuo-Chen Li, Jing-Yuan Chen
Magmatic activity in the syn-collision stage is key for net crustal growth. To understand the mechanism of accretion–differentiation and compositional change of the continental crust, it is important to focus on the magmatic activity during the syn-collision stage. Early Eocene mafic–ultramafic rock assemblages found in the western part of the Tengchong Block resulted from a continuous series of arc magmatic evolution, thoroughly recording the continental arc magmatic system during the subduction of the Neo-Tethys Ocean and syn-collision of the Indian-Asian continents. Early Eocene hornblende gabbro–diorite in the Tengchong Block formed at 53 Ma, and the primitive magma was derived from an enriched mantle source due to the enriched Nd–Hf isotopes. The amphibole and biotite thermobarometer measurements indicate that the mafic magma reservoirs in the Tengchong Block occurred at a mid-upper crust. Petrography, amphibole Fe/Mg exchange coefficient (KD), Rayleigh fractionation, and equilibrium melt calculation indicate that the Early Eocene hornblende gabbro–diorite in the Tengchong Block was created due to plagioclase-dominated accumulation at the mid-upper crust level. Based on the calculation, the corresponding amphibole equilibrium melt is more silicic (dacitic–rhyolitic in composition) than the bulk rocks, indicating a more evolved composition in the mid-upper crust. Three types of plagioclases reveal the multi-recharging and dissolution–reprecipitation promoting the further evolution of these mafic rocks. Therefore, this study concludes that magma recharge and plagioclase-dominated accumulation processes may be important mechanisms for the formation and evolution of mafic magma and the further crustal differentiation at the mid-upper crust level in a continental margin arc.Arc is an important region for the growth and differentiation of the continental crust, and arc igneous rock is ideal for understanding the evolution of magma reservoirs and the transcrustal magmatic system in depth. Increasing level of attention is being given to the evolution process and the corresponding mechanism of magmatism in the continental arc [1-6]. However, the andesitic component of the continental crust cannot be completely derived from the single-stage melting of mantle-derived magmas; it requires additional magmatic evolutionary processes. These processes include gradual differentiation of mantle-derived basaltic magmas by fractional crystallization within the upper mantle and lower crust, and/or partial melting of the early mafic crust [1, 2, 7-10]. Recently, studies on the construction and differentiation of the continental crust have focused on the genesis of granite [11-16], whereas the vertical multistage differentiated evolution of mantle magma within the continental crust can be considered as the fundamental process of magmatic evolution from the mafic lower crust to the felsic upper crust [7, 8, 17-19]. The pyroxene-/amphibole-rich mafic intrusive and ac
一些科学家认为,源于地幔的含水玄武岩浆通过部分结晶形成了岩浆积层[32-35],而另一些科学家则认为,地壳中的岩浆岩是部分熔融、地壳污染和/或弧壳内岩浆混合的残留物[1, 36]。弧岩浆演化的跨地壳岩浆系统表明,源自地幔的岩浆通过晶体堆积和从不同深度相连的岩浆库中提取熔体而分层,导致岩浆成分从岩浆岩向硅质岩演化,演化过程中可能涉及同化物污染和其他过程[5, 37, 38]。实验岩石学和自然研究也表明,含水黑云母-超黑云母岩浆的形成是由于地壳不同深度矿物组合的多巴分化[33, 39]。因此,系统研究同步碰撞阶段大陆边缘弧内岩浆侵入体的成因,对揭示岩浆储层特征,进一步查明大陆弧地壳岩浆演化和垂直分异具有重要意义。腾冲地块是与新泰西洋东俯冲有关的倾斜大陆边缘弧[27, 28, 40-43]。中新生代岩浆岩被认为是冈底斯岩浆弧的东南延伸,在腾冲地块西部发现的大量完整的早新生代黑云母-超黑云母岩石组合是典型的大陆边缘弧侵入岩,处于与印度-亚洲大陆碰撞有关的同步碰撞阶段(50、55Ma)[13、42、43]。出露的岩石类型主要为角闪岩、角闪辉长岩和闪长岩,不同的岩性代表了不同深度的黑云母岩浆系统演化的产物。以往关于不同岩浆岩成因的研究,将俯冲带不同成岩介质造成的源区性质差异归因于这些岩浆岩之间的差异[42, 43]。然而,地壳内部的演化过程,尤其是分异过程,对岩浆岩的岩石成因和地球化学性质也起着重要作用。因此,本研究选择了腾冲地块西部的龙蟠角闪辉石-闪长岩作为研究对象。通过岩石学、年代学、全岩地球化学、Sr-Nd同位素组成、锆石的Lu-Hf同位素、斜长石的Sr同位素以及主要成岩矿物的主要元素和微量元素分析,探讨了这些岩浆岩的成因、演化及其在弧岩浆系统中的作用。结果表明,腾冲区块的早始新世角闪辉石-闪长岩是大陆弧岩浆系统中地幔源岩浆演化的产物;结果表明,它发育于地壳中上部,经历了以斜长石为主的堆积过程,可能是同步碰撞阶段大陆弧地壳中上部化学分异的一个有效过程。腾冲地块位于三江四迭造山带西南缘,延伸至青藏高原拉萨地块东南缘[44-47]。腾冲地块西接缅甸西地块的茂谷变质带和实皆断陷,东邻保山地块的高黎贡山带(图1(a))。腾冲地块具有中新生代-新元古代变质基底-高黎贡组,上部为变质、硅质、片麻岩,下部含少量黑云母-超基性花岗岩[46,47]。腾冲地块是西布玛苏地块的一员,在古生代早期形成冈瓦纳大陆的北缘,在中生代晚期冈瓦纳大陆解体后与欧亚大陆拼接[42, 47]。白垩纪晚期-始新世早期的新特提斯洋经历了向东俯冲和闭合的过程,在腾冲地块的盈江-龙川地区形成了大量的岩浆-长石弧岩浆岩[27, 28, 48-50]。龙蟠地区位于腾冲地块西部,是早更新世西马-通背关花岗岩岩体(图 1(b))的邻近地区,岩石以小储量形式出露。岩性主要包括角闪辉长岩和闪长岩(图2(a)-(c)),质地为中-细粒。岩相学显示了以斜长石和闪长石为主的积层结构。
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引用次数: 0
On the Influence of Grain Size Compared with Other Internal Factors Affecting the Permeability of Granular Porous Media: Redefining the Permeability Units 与影响粒状多孔介质渗透性的其他内部因素相比,粒度的影响:重新定义渗透率单位
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-01-12 DOI: 10.2113/2024/lithosphere_2023_231
Jesús Díaz-Curiel, Bárbara Biosca, Lucía Arévalo-Lomas, David Paredes-Palacios, María J. Miguel
This study first reviews the influence of grain size on the permeability of porous granular media in comparison to other factors, especially the sorting of grain size distribution, in order to improve the physical knowledge of permeability. The aim of this research is to counter the widespread misconception that the characteristics of water flow in granular porous media can be associated exclusively with an area regarding grain size. This review involves two different aspects. First, the dependence of the intrinsic permeability on the particle size distribution is highlighted, independently of the other internal factors such as porosity and average grain size, by simply reviewing the main existing formulas. Second, the historical literature on the influence of the average grain size in porosity is analyzed, and it is compared with the influence of the granulometric sorting. The most recognized data show that the influence of each of these two factors is of the same order, but it was not expressed in mathematical form, so a relationship of porosity versus average grain size and sorting is established. The two aforementioned steps conclude that the factors influencing permeability do not advise the use of area dimensions because it leads to only link permeability with the average grain size, especially when nonspecialists come into contact with earth sciences. Finally, after a review of the historical evolution of the permeability units, they are redefined to avoid the common misconception that occurs when the established unit leads to only a partial understanding of the key parameters influencing permeability.Historically, permeability characterizes all types of porous solid media, focusing this work on granular media, where permeability is a key petrophysical parameter due to its application in many fields of Earth sciences, such as hydrogeology, oil field, geological environment, geotechnics, and soil science in agronomy.As initially established by Darcy [1], permeability is the ease with which water can move through pore spaces in porous media. The flow velocity of water depends on the internal characteristics of the medium and the pressure gradient to which it is subjected; however, considering the rigidity of the solid phase, in granular media, this flow velocity depends on the pressure gradient to which the water is subjected [2].Over time, the concept of permeability long included the influence of temperature, which was first recognized at the same time as the concept of fluid viscosity [3, 4]. In this way, by including the fluid viscosity in the relationships to obtain permeability, a process to generalize the Darcy equation to the flow of any fluid was initiated. However, this process implied the separation of two very distinct aspects affecting the measurable flow velocity, the internal characteristics of the medium, and the characteristics of the fluid. Despite this, the term permeability was maintained up to 1940 to characterize flow i
因此,本研究给出的与多孔介质中的流动相关的新术语和单位的重新定义是对原始概念的尊重,符合必要的科学严谨性,并与这些常用关系完全对应[1, 2]。此外,与 1940 年建立的术语不同,这些术语是一套结构清晰的新术语。与现有术语的区别在于回归了渗透率的原始概念,从而摒弃了哈伯特[71]提出的修改建议,他用 "流体导电率 "来反映渗透率,用 "渗透性 "来反映通常所说的固有渗透率。此外,这套新单位与传统单位的主要区别在于,采用了无量纲压力梯度下 1 达西 = 1 厘米/秒的渗透率原始单位,而不是 Wyckoff 等人[70]给出的压力梯度为 1 atm/cm 时的 1 达西定义。同样,根据 Kozeny [2] 等人的方程得出的 1 cm/s ≡ 10-2 cm2 的等量关系也被采用,从而摒弃了 Hubbert [73] 确立的 1 cm/s ≡ 10-8 cm2 的等量关系,这与目前使用的等量关系存在巨大差异。与达西之后的文献中确定的渗透率单位相比,达西方程中对渗透率速度单位的导数分配使其成为一个易于测量的参数,可提供与颗粒多孔介质中的流动直接相关的数值。水导也是如此。此外,与理解使用面积单位在概念上的复杂性相比,处理速度单位的倍数则简单明了。固有渗透率(或水力传导率)同时提供了与流体类型无关的数值;但是,它不能阐明多孔介质中的实际流动情况,因为它不能将水与其他流体(如油)区分开来。此外,它提供的数值的面积尺寸与介质的任何现有表面都不一致。因此,颗粒介质中渗透率与颗粒(或孔隙)大小之间的联系导致了对渗透率概念的误解。我们的重新定义与渗透系数(自达西[1]以来)和本征渗透率(自科泽尼[2]以来)的历史定义相吻合。不过,本研究证明了它们之间的等效性。新的导水性概念和对导水性的重新定义是以国际单位制的一般划分为基础的;粘度不同于水的流体在颗粒状多孔介质中的流速取决于渗透率和压力梯度(如达西方程[1]),流体粘度以最简单的方式加入其中(方程 8),介质的结构特征通过本征渗透率和导水性反映出来,作为压力梯度的单位。采用所提议的单位将有助于推进动态渗透率估算技术(即作者声明,本文的发表不存在任何利益冲突。本研究的部分工作得到了马德里大区政府的支持(CARESOIL-CM 项目资助编号 P2018/EMT-4317)。
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引用次数: 0
Controls of Multi-Scale Fractures in Tight Sandstones: A Case Study in the Second Member of Xujiahe Formation in Xinchang Area, Western Sichuan Depression 致密砂岩中多尺度断裂的控制:四川西部凹陷新昌地区徐家河地层第二层实例研究
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-01-12 DOI: 10.2113/2024/lithosphere_2023_343
Junwei Zhao, Yingtao Yang, Gongyang Chen, Xiaoli Zheng, Senlin Yin, Lei Tian
Different scales of fractures affect the reservoir quality in tight sandstone. There are more studies on macroscopic tectonic fractures but less on bedding fractures and microfractures. The control factors of multi-scale fractures are unclear. In this paper, we analyzed the types and controls of fractures in the second member of the Xinchang region in Western Sichuan. We use core and outcrops observations, imaging logging, scanning energy spectra, and rock slices. Natural fractures can be classified into tectonic, bedding, and microscopic types. The tectonic fractures are mainly low- to medium-angle tensile fractures. The bedding fractures are nearly horizontally distributed along the bedding surface, including parallel, dark mineral interface, and carbonaceous fragments interface bedding fractures. The microfractures develop intra-grain, edge-grain, and inter-grain types. The intra-grain microfractures are inside quartz or feldspar grains, whereas inter-grain types penetrate multiple grains with larger extension lengths. The tectonic fractures are related to the stress, grain size, mineral component, argillaceous content, and lithologic thickness. Parallel bedding fractures are controlled by the coupling of water depth and flow velocity. Bedding fractures at the interface are controlled by rock component. The microfractures are controlled by the length-width axis ratio of the grain, grain element content, and brittleness index. Fractures of different scales form a three-dimensional fracture system that has a substantial impact on the gas production.Tight sandstone gas is an unconventional natural resource dominated by low-porosity and low-permeability reservoirs with porosity less than 10% and air permeability less than 1 × 10–3 μm2 [1-4]. It has been discovered in many basins in China [5-8] and accounts for a relatively large proportion of the gas production, such as in the Ordos, Sichuan, Junggar, and Tarim basins [9-16]. The Xinchang gas field in the Sichuan Basin was first discovered in 1988. The exploration progress was slow owing to the insufficient understanding of geological and fracking processes. After 2,000 years, a few exploration wells were drilled in close to the fracture system, and gas production was increased [17-21]. Exploration showed that the fractures play an important role in controlling the gas production of the Xinchang gas field. However, the distribution of fractures in this zone is complex with different fracture geneses, scales, and occurrences. Nevertheless, there is a lack of the systematic understanding of fractures.Tectonic fractures in tight sandstones have been extensively studied [22, 23]. The factors affecting them include the stress heterogeneity in different tectonic zones [24-31] and lithologic heterogeneity [32-34]. Sedimentation controls differences in the lithology and layer thickness, and heterogeneity in the mineral composition and structure of reservoirs influence fracture development [35-40]. Bedding
新昌构造带第二段的这些断裂受多种因素控制。构造应力是主要因素,同时与岩性、地层厚度和力学层密切相关。构造应力差控制着这些裂缝的发育。储层中的这些断裂表明,越靠近大断层,构造断裂越发育(图 14)。例如,距离大断层约 2600 米的 X11 井的平均裂缝线密度为 0.21 米-1,而距离大断层约 400 米的 X501 井的平均裂缝线密度为 1.83 米-1。研究区内较好的产气井一般位于主断层或小褶皱轴线附近。断层活动使断裂带受到明显的应力集中现象,断裂带附近的断裂较为发育。因此,构造带的差异和与主断层的距离控制着储层的构造应力,进而影响构造裂缝线密度。岩性差异影响着储层裂缝的发育,岩性通过粒度、矿物组分、胶结物和钙质胶结物含量影响裂缝。不同岩性的裂缝线性密度统计结果显示,粒度与平均线性密度之间存在一定的关系(图 15)。例如,X501 井中砂岩的线密度较大,高达 1.83 m-1,而细砂岩的线密度较小。储层的晶粒成分多种多样,其弹性模量和泊松比也大不相同,因此在相同应力下会形成不同的裂缝。例如,X201 井中石英砂岩的线密度较大,可达 0.83 m-1,而石质砂岩的线密度较小,约为 0.1 m-1。脆性矿物含量较高,有利于构造裂缝的发育。这些断裂的有利岩相类型是石英砂岩。箭石含量也会影响断裂。为了排除粒度和矿物成分的影响,我们选择了 X501 井中粒度和成分相似的地层来讨论箭石含量对构造裂缝的影响。可以看出,箭石含量与构造裂缝线密度呈负相关(图 16)。岩石力学层是指岩石力学性质相同或相似的岩性层。这些岩层一般终止于泥岩界面。构造裂隙通常发育在岩石力学层内部,很少有裂隙能穿过泥岩层[74]。可以发现,岩层厚度与断裂线密度之间存在着很大的关系。为了消除岩性的影响,对中砂岩的断裂线密度进行了分析。从图中可以明显看出,它呈现出一定的相关性(图 17),线性密度随着岩层厚度的增加而减小,每口井都存在一个厚度临界值,超过这个临界值,随着岩层厚度的增加,压裂线性密度变化不大。小于该临界值时,随着厚度的减小,压裂线密度在一定范围内会变大。它们的形成主要归因于沉积作用和成岩作用,而构造作用则是诱发因素[48]。对于这些断裂,沉积物在成岩过程中受到上覆地层压力的持续增加,不同类型的层理界面上的沉积物颗粒经历了不同的压实和胶结作用[48],如深色矿物界面和浅色矿物界面。两种矿物的压实压力并不一致,在成岩过程中,裂缝沿层理界面分布。由于类似的原因,平行层理由不同粒度的岩层组成。层与层之间的粒度存在差异。此外,不同粒度的层在成岩过程中的压实过程也存在差异,粗粒的抗压实能力强,细粒的抗压实能力弱。压实发生在细粒层的界面上,形成机械薄弱面和平行的层理断裂,形成剥蚀线状结构。这些在成岩过程中形成的断裂受到构造应力的作用。断裂的尺度在一定程度上发生了改变。因此,层理断裂受内生因素控制。
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引用次数: 0
Influence of the Advance Jacked Pipe on the Jacking Force of the Subsequent Pipe Based on Pipe–Soil Full Contact Model 基于管道与土壤完全接触模型的先行顶管对后行顶管顶力的影响
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-01-12 DOI: 10.2113/2024/lithosphere_2023_216
Yu Zhang, Xu Zhao, Fei Guo, Lianjin Tao, Jun Liu, Weizhang Liao, Lei Tan, Xiaohui Yang
In pipe jacking engineering, accurate prediction of jacking force is the key to pipe jacking design. Based on a project of the Beijing Daxing Airport Line, the influence of the advance jacked pipes on the jacking force of the subsequent pipe is carried out in the present work. First, the verified numerical model of practical engineering was established, and the jacking force and radial stress of different pipes were analyzed. Then, the two pipes were taken as research object, and the parameters of spacing, angle, buried depth, and pipe diameter were investigated, respectively. The results show that in the actual project, the advance jacked pipes have amplification and superposition effects on friction resistance of the subsequent pipe, and the maximum growth rate is 37.2%. The friction resistance of the subsequent pipe presents a trend of first increasing and then decreasing with the change of the layout angle of advance jacked pipe from 0° to 180°. With the increase of buried depth and pipe diameter, the absolute value of incremental friction resistance of the subsequent pipe increases gradually, but the growth rate remains constant. Finally, the empirical formulas for predicting the friction resistance growth rate of subsequent pipes under different angles are proposed. The research results can provide some reference for the design of pipe jacking.In recent years, rapid urbanization resulted in a great development in underground space. The pipe jacking method has been widely used in energy transportation engineering, water conservancy, and tunnel engineering because of its advantages of fast construction speed, little disturbance to the surrounding environment, and easy-to-control jacking accuracy [1-12]. Besides, pipe jacking is also used in pipe roof engineering. For example, the Xinle Ruin station of Shenyang subway line 2 was built with the pipe roof method. The pipe roof structure consists of 19 steel pipes with a diameter of 2000 mm and 2 steel pipes with a diameter of 2300 mm [13]. The Gongbei tunnel was built by 36 steel pipes with a diameter of 1620 mm [14].The core problem of pipe jacking is still the calculation of friction resistance. The magnitude of the jacking force is directly determined by the friction resistance, and the radial stress of the pipe–soil interface determines the distribution and magnitude of friction resistance stress. At present, the existing literatures have done a lot of research on the friction resistance. The numerical simulation and laboratory test methods have been adopted to study the pipe–soil interaction under different types of lubricants and their combinations by Shou et al. [15]. They concluded that the reduction of the jacking force is closely related to the decrease of friction coefficient, and the effect of lubrication is slightly more significant in the case of curved pipe than in the case of linear pipe. Yen and Shou [16] took the obtained average friction coefficient as the input parameter of t
随着顶管间距的增大,后续管道摩擦阻力的绝对值增量和增长率逐渐减小。随着埋深和管径的增大,后续管道摩阻增量的绝对值逐渐增大,但后续管道摩阻的增长率保持不变。国家自然科学基金(42072308)、国家重点研发计划(2019YFC1509704)、北京土木建筑大学青年教师科研能力提升计划(批准号:X23005)和北京市市政工程研究院资助了本研究。我们非常感谢这些资助。
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引用次数: 0
Influence of Lithology on the Characteristics of Wave Propagation and Dynamic Response in Rocky Slope Sites Subject to Blasting Load Via the Discrete Element Method 通过离散元素法研究岩性对受爆破荷载影响的岩石边坡场地的波传播特征和动态响应的影响
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-01-12 DOI: 10.2113/2024/lithosphere_2023_302
Danqing Song, Xuerui Quan, Zhuo chen, Dakai Xu, Chun Liu, Xiaoli Liu, Enzhi Wang
To investigate the dynamic response and attenuation law of rock slope sites subjected to blasting, three lithological numerical models, including slate (hard rock), tuff (relatively soft rock), and shale (soft rock), are established by using MatDEM. By analyzing the wave field, velocity, and acceleration response of the models and their Fourier spectrum, combined with stress and energy analysis, their dynamic response characteristics are investigated. The results show that blasting waves propagate from near field to far field in a circular arc, and the attenuation effect of waves in soft rock is less than that in hard rock. The influence of lithology on the dynamic response of the ground surface and bedrock is different. Blasting waves mainly affect the dynamic response in the near-field area of the blasting source. In addition, the dynamic amplification effect of slopes is as follows: hard rock > relatively soft rock > soft rock. The slope surface has an elevation attenuation effect. A dynamic amplification effect appears in the slope interior within the relative elevation (0.75, 1.0). The Fourier spectrum has an obvious predominant frequency, and that of the slope crest and interior is less than that of the slope surface. Moreover, the total energy generated by the rocky sites gradually changes into kinetic energy, gravitational potential energy, elastic potential energy, and heat. Energy-based analysis shows that the attenuation effect of blasting waves in hard rock is larger than that in soft rock overall. This work can provide a reference for revealing the blasting vibration effect of rock sites.Because of the advantages of fast construction, low cost, and high efficiency, the blasting method has become the main construction method of slope and tunnel engineering [1]. Nevertheless, due to the influence of the propagation medium, the waveforms and propagation characteristics of blasting seismic waves become very complicated [2]. Blasting seismic waves will lead to slope instability and other geological disasters; in particular, in coal mining areas, under the influence of human blasting over the years, geological disasters, such as mountain cracking and creep, will occur on slopes, seriously threatening the safety of people’s lives and property [3, 4]. Moreover, seismic exploration blasting technology is an important method in geophysical exploration [5]. The seismic effect of explosive blasting has become a key problem in land oil and gas exploration and foundation construction. The propagation law and damage effect of seismic waves in different geological bodies are the main basis of engineering blasting design [6, 7]. Therefore, explosion-induced seismic waves have been one of the most active subjects in the field of civil engineering blasting.Blasting seismic waves are a complex physical phenomenon [8, 9]. It is affected by many factors, such as the location of the source of detonation, the amount of explosive, the mode of explosion, the
在爆破作用下,不同岩层产生的总能量会逐渐转化为动能、重力势能、弹性势能和热能。岩性对岩场产生的总能量和机械能有影响:硬岩 > 相对软岩 > 软岩。爆破地震波在硬岩场的衰减效应大于软岩场。爆破波以震源为中心,从近场到远场呈现圆弧衰减传播特征。斜坡的动态衰减效应大于地表的动态衰减效应。岩性影响模型中波的传播速度和振幅。软岩中波的传播速度大于硬岩,软岩中波场的衰减传播特性小于硬岩,岩性对地表和基岩中波的动态响应特性有不同的影响。在地表,硬岩的动力放大效应小于软岩,硬岩的衰减率大于软岩。波在基岩中的衰减效应在硬岩中小于软岩。爆破荷载主要影响爆破源近场区域的动态响应,而对远场区域影响不大。在近场区域,波在地表似乎具有快速衰减效应(相对软岩 > 软岩。软岩斜坡的动态衰减效应大于硬岩斜坡。高程对波浪有明显的衰减作用,在 h/H = 0-0.2 范围内衰减率最大。在斜坡内部,在 h/H = 0-0.75 范围内首先呈现动态衰减效应,在 h/H = 0.75-1.0 范围内呈现放大效应。在坡顶,随着与坡肩距离的增加,先放大后衰减。岩性对爆破源地表和基岩的傅立叶频谱特征影响较小,但对边坡的傅立叶频谱特征影响较大。应力和能量分析表明,爆破波主要在地表和边坡区域产生拉应力,在深部基岩产生压应力。爆破荷载对模型底界的动力响应影响较大,硬岩场底界的法向应力大于软岩。在爆破作用下,不同岩场产生的总能量逐渐转变为动能、重力势能、弹性势能和热能。岩性对岩石部位产生的总能量和机械能有影响:硬岩 > 相对软岩 > 软岩。通过 MatDEM 在时域和频域研究了岩石边坡场地的动态响应特征和衰减规律,讨论了爆炸地震波在岩石边坡场地从近场到远场的传播和波形特征,揭示了岩性对爆破下岩石场地动态响应特征的影响。宋丹青:方法学、调查、可视化和写作-原稿。Xuerui Quan:软件、数值建模和写作-原稿(数值建模)。陈卓:构思和指导。本研究得到了国家自然科学基金(52109125、52208359 和 41941019)、中央高校基本科研业务费(2023ZYGXZRx2tjD2231010)、江苏省自然科学基金(批准号:BK20231217)、国家自然科学基金(批准号:BK20231217)的资助。BK20231217)、科技服务网络行动(2022T3051)和四川省自然科学基金(24NSFSC4541)。 在最基本的线性弹性模型中,假定颗粒依靠弹簧相互接触并产生力。粒子间的法向力(Fn)和法向变形(Xn)可以用粒子间的法向弹簧来模拟[34]:其中 Kn 是法向刚度,Xn 是法向相对位移(图 1(b)),Xb 是断裂位移。最初,颗粒与相邻颗粒相连,并受到拉力或压力弹簧力的作用。当两个颗粒之间的 Xn 超过断裂位移(Xb)时,弹簧断裂,颗粒之间的拉力消失。切向弹簧用于模拟颗粒间的剪切力(Fs)和剪切变形(Xs)[35]:其中 Ks 为切向刚度,Xs 为切向位移。同样,在弹簧的切割方向上也有一个失效准则,该准则基于莫尔-库仑准则[34, 35]:其中 FSmax 是最大剪切力,FS0 是颗粒间的剪切阻力,μp 是颗粒间的摩擦系数。在莫尔-库仑准则中,单元间的最大剪切阻力与初始剪切阻力 (Fs0) 有关。Fs0 是在不施加法向压力的情况下,单元间可承受的最大剪切力,与岩土体的内聚力类似。法向压力越大,剪切阻力越大。当切向力超过最大剪切力时,切向连接断裂,颗粒之间只存在滑动摩擦力 -μp-Fn。在数值模拟中,引入了法向弹簧和切向弹簧,以平衡现实世界中颗粒之间的胶结,如砂砾石和其他沉积物在成岩过程中沉积时的铁质胶结和钙质胶结。因此,当数值模拟中的法向弹簧断裂时,就相当于现实世界中的胶结断裂。此时,切向弹簧也应断开,反之亦然[33,36]。由线性弹性接触定义的单元堆积模型具有整体的弹性特征。如果要模拟材料的弹塑性和蠕变特性,则需要定义不同的接触模型。例如,对于弹塑性材料,元件也需要定义为近似弹塑性。宏观和微观研究是 DEM 的一个非常重要的分支,即如何根据材料的宏观力学性能建立合适的单元接触模型并确定相应的参数[37, 38]。上述刚度是元素之间连接的刚度(Kn),每个元素都有自己的刚度(Kn)。当两个元素接触时,实际上是两个弹簧串联。对于法向刚度为 Kn1 和 Kn2 的两个元素,其连接的等效法向刚度(Kn)为 [33, 36]:对于切向刚度为 Ks1 和 Ks2 的两个元素,其连接的等效切向刚度(Ks)为 [33, 36]:同样,每个元素都有自己的断裂位移和摩擦系数,连接的机械性能取决于较小元素的抗拉或抗剪能力。因此,如果两个元件的刚度相同,则串联连接的刚度(Kn,Ks)是元件刚度(Kn,Ks)的一半,串联连接的断裂位移(Xb)是元件断裂位移(Kb)的两倍。在数值计算中,使用构件的刚度和断裂位移,并通过计算获得连接的力学性能。在每个质点受力的基础上,通过时间步长迭代算法计算质点的位移。设置时间步长 dT,计算质点的力、加速度、速度和位移。当前时间步计算完成后,再前进一个时间步,实现 DEM 的迭代。具体步骤如下:基于传统的牛顿力学方法,在已知每个粒子所受结果力的基础上,用结果力除以粒子质量,得到此刻粒子的加速度。在时间步长 dT 中,将当前速度加上速度增量。也就是说,可以得到下一个时间步的初始速度,并通过时间步内的平均速度计算出相应的元素位移。然后,通过反复迭代进入新的迭代计算,实现 DEM 动态模拟。
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引用次数: 0
Experimental and Numerical Investigation of Rock Failure Process under Hydromechanical Coupling Action 水力机械耦合作用下岩石破坏过程的实验和数值研究
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-01-12 DOI: 10.2113/2024/lithosphere_2023_317
Zeqi Zhu, Xiancheng Mei, Jianhe Li, Qian Sheng
In order to study the initiation mechanism of rocks under hydromechanical coupling, hydromechanical coupling triaxial tests and acoustic emission tests were carried out on basalt in the Xiluodu hydropower station dam site area in southwestern China. The test results indicate that the basalt displays typical hard brittle behavior, and its peak strength increases as confining pressure rises. Conversely, the peak strength decreases gradually as the initial water pressure increases, which leads to decreased hardness. Meanwhile, tensile failure is the main crack initiation mode under hydromechanical coupling action. During the stable crack growth stage, tensile failure is predominant, complemented by shear failure, with failures mainly occurring in the rock middle position. Contrary to this, during the unstable stage, the rock failure is mainly due to shear failure. The critical pore water pressure failure criterion of rock crack initiation under hydromechanical coupling conditions is derived based on the test results and introduced into the numerical simulation. The hydromechanical coupling failure process and pore water pressure distribution law of basalt are analyzed, and the rationality of the critical pore water pressure failure criterion is verified. These findings are significant for understanding the rock failure process under hydromechanical coupling action and provide a valuable reference for future research.Hydroelectric engineering projects often involve structures such as underground power stations, water diversion tunnels, and sloping dam foundations, which are subjected to the combined action of high-ground stress and strong osmotic pressure. Therefore, research on the mechanical properties of rocks or rock masses under hydromechanical coupling has become a pressing issue in geotechnical engineering. Several scholars, including Song et al. [1], Zhu et al. [2], Yu et al. [3], Xu et al. [4], Wang et al. [5], and Wang et al. [6], have conducted hydromechanical coupling triaxial tests on limestone [1-3], sandstone [4-6], and granite [7, 8] to investigate the relationship between rock permeability, stress, strain, and pore water pressure. They have discussed the influence of pore water pressure on rock strength characteristics, deformation laws, and damage evolution. Moreover, Li et al. [9], Zhao [10], and Guo et al. [11] have employed acoustic emission (AE) signals to analyze the AE characteristics during the process of rock cracking under hydromechanical coupling.The aforementioned research has extensively demonstrated that hydromechanical coupling induces pore water pressure within the internal cracks of a rock, which significantly impacts the cracking process [12, 13]. Once the pore water pressure attains a critical level, it instigates the inception, expansion, and penetration of rock cracks, commonly referred to as hydromechanical fracturing [14]. This phenomenon is a significant factor that causes a range of engineering disasters, inc
在峰值强度和峰值后阶段,岩石内部的孔隙水压力分布发生了显著变化。除下端面外,其他位置的孔隙水压力耗散非常明显,并趋向于零。本研究选取溪洛渡玄武岩为研究对象,通过水力机械耦合三轴试验、AE 试验和数值模拟分析,得出以下结论:水力机械耦合三轴试验表明,在初始水压不变的情况下,玄武岩的峰后应力下降明显,峰值强度随约束压力的增加而增加,表现出典型的硬脆行为。当约束压力保持不变时,随着初始水压的增加,峰值强度逐渐降低,应力降减弱,这意味着水压在一定程度上削弱了岩石的抗压强度,使其硬脆性减弱。在裂纹稳定扩展阶段,拉伸破坏是主要破坏模式,剪切破坏是辅助破坏模式。这些破坏主要发生在岩石中部。根据 AE 试验的结果,建立了水力机械耦合下的裂缝破坏计算模型,并得出了裂缝起始的临界水压破坏准则。将临界水压破坏准则纳入玄武岩水力机械耦合三轴试验的数值模拟中,模拟结果与试验结果基本一致。水力学耦合三轴试验表明,在初始水压不变的情况下,玄武岩的峰后应力下降明显,峰值强度随约束压力的增加而增加,表现出典型的硬脆行为。当约束压力保持不变时,随着初始水压的增加,峰值强度逐渐降低,应力降减弱,这意味着水压在一定程度上削弱了岩石的抗压强度,使其硬脆性减弱。在裂纹稳定扩展阶段,拉伸破坏是主要破坏模式,剪切破坏是辅助破坏模式。这些破坏主要发生在岩石中部。根据 AE 试验的结果,建立了水力机械耦合下的裂缝破坏计算模型,并得出了裂缝起始的临界水压破坏准则。将临界水压破坏准则纳入玄武岩水力机械耦合三轴试验的数值模拟中,模拟结果与试验结果基本一致。这揭示了玄武岩水力机械耦合断裂的过程和水压分布的规律,验证了临界水压失效准则的合理性。本研究得到了国家自然科学基金项目(U21A20159、52009129)、水利部水网工程与调控重点实验室项目(QTKS0034W23291)和水利工程与管理国家重点实验室客座研究员基金项目(2023SGG07)的资助。作者衷心感谢所有给予我们帮助和合作的成员。
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引用次数: 0
Gravity-Seismic Joint Inversion of Lithospheric Density Structure in the Qiongdongnan Basin, Northwest South China Sea 南海西北部琼东南盆地岩石圈密度结构的重力-地震联合反演
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-01-12 DOI: 10.2113/2024/lithosphere_2023_124
Chaoyang Li, Wei Gong, Lihong Zhao, Zhonghua Li, Pengyao Zhi, Jiayu Ge
Qiongdongnan Basin (QDNB), located at the northwestern corner of the South China Sea (SCS), is a key juncture between the extensional tectonic regime in the northern continental margin and the shear tectonic regime in the western continental margin. Analyzing the crustal density structure and tracking the thermodynamic controlling factors are effective approaches to reveal the nonuniform breakup process of the northwestern SCS. Herein, focusing on the obvious tectonic deformation with distinct eastern and western parts in the QDNB, we present the crustal density structures of five profiles and identify the high-density anomaly related to the synrifting mantle underplating and postrifting magmatic intrusions. The crustal density model was constructed from the Bouguer gravity anomaly, ocean bottom seismic profiles, and multichannel seismic reflection profiles. The northern part of QDNB, with normal crustal density, lower surface heat flow of <55 mW/m2, and limited extension factor of 1.25–1.70, is recognized as the initial nonuniform extension continental crust. The mantle underplating beneath the QDNB is identified as a high mantle density of 3.30–3.40 g/cm3 and a high lower crustal density of 2.92–2.96 g/cm3, which is usually recognized by the high-velocity layers in the northeastern margin of SCS. The magmatic intrusions are identified as the high-density bodies ranging from 3.26 g/cm3 at the base to 2.64 g/cm3 at the top, which become stronger from the west to east. The central part of Xisha Trough is featured by the cooling of the heavily thinned lower crust in the final continental rifting stage, which is close to the cold and rigid oceanic crust. Lateral variations in the deep magmatic anomaly should be the crucial factor for the nonuniform breakup process in the northwestern margin of SCS.As the largest Cenozoic marginal basin located in the western Pacific region, the South China Sea (SCS) was formed in a complex tectonic setting due to the strong interaction among the Indo-Australian, Eurasian, and Pacific plates [1, 2] (Figure 1). Because of the stretching stress introduced by the rollback of the paleo-Pacific plate and the slab pull of the paleo-SCS, the SCS shows the ununiform continental rifting and progressive seafloor spreading from east to west, featuring highly inhomogeneous crustal structure and asymmetric magmatism beneath the marginal basins [3-5]. It is generally accepted that the SCS might represent a “plate-edge or Pacific-type” extensional basin, and the passive upwelling of the fertile asthenospheric mantle induced by the surrounding subductions could be primarily responsible for these inhomogeneous features [6, 7]. Some scholars even believed that the SCS had experienced a “magma-rich”-type breakup process in its middle-eastern part, but a “magma-poor” one is observed in the west [4, 8].In the case of the northern continental margin of SCS, the compositional or structural east–west heterogeneity has been observed by vario
这些区域显示出岩浆成分的特征,更接近大洋地壳。同样,上地幔的密度从南北两肩的 3.00-3.21 克/立方厘米到中部盆地的 3.30-3.40 克/立方厘米有较大的增加,这是最明显的深岩浆异常指标。火成岩斜长岩也被认为是高密度岩体,从底部的 3.26 克/立方厘米到顶部的 2.64 克/立方厘米不等。火成岩可能与来自上地壳或沉积物的低密度体混合在一起。此外,地表热流数据也被投射到剖面上,以帮助确定岩浆活动异常的范围[59]。QDNB 西部的地貌特征包括非对称地堑、上地壳高角度正断层、下布盖尔重力异常、有限的低角度剥离以及轻微的断裂后岩浆活动[15, 21, 35, 36, 60](图 1 和图 2)。由于地壳减薄程度不同,地壳密度沿剖面 L1-L2 显示出显著变化。在乐东下陷、陵水下陷和剖面L1南段观察到强烈的地壳延伸,地幔隆起3-5 km,热流高达65-80 mW/m2,延伸因子大于3.00[36, 41](图4)。3.40克/立方厘米的地幔高密度体位于地壳强烈延伸区的下方,这可能与深部岩浆上涌有关。在下地壳底部也发现了类似的 2.92-2.96 克/立方厘米的高密度体,这可能与同步移动阶段的地幔下沉有关。这些下地壳高密度体通常被认为是在珠江口盆地和台西南盆地下广泛观测到的高密度低地壳的典型特征[6, 9]。剖面 L1 北部的崖北下陷和崖南下陷以及剖面 L2 南部的西沙隆起仍保持大陆地壳的正常密度,其有限延伸系数为 1.25-1.70 [35,36]。横跨秦岭北麓东部的L3-L5剖面显示出明显不同的地壳结构,复合对称地堑、高度发育的剥离断层深入地壳下部,以及广泛的断裂后岩浆活动[15, 21, 35, 36, 60](图1和图3)。秦岭北麓东部的地壳延伸和地幔下伏似乎更为强烈,在大部分地区的下地壳和上地幔下广泛分布着2.92-2.96和3.30-3.40 g/cm3的高密度体(图4)。在西沙海槽中部,沿剖面 L4 的过伸地壳厚度甚至接近 0 公里。地幔隆起和热流在秦岭北麓东部地区分别高达10千米和120毫瓦/平方米,明显高于秦岭北麓西部地区。只有在 L4 剖面的北部和 L5 剖面的神湖隆起区观测到正常密度的大陆地壳。秦岭北麓东部最显著的特征是大规模的漂移后火成岩斜长岩,密度为2.63-3.26克/立方厘米。沿剖面 L5 观察到的火成岩侵入体比沿剖面 L3-L4 观察到的更强烈,密度更高,为 2.94-3.26 g/cm3。此外,值得注意的是,尽管各层设置了密度上限,但沿剖面 L5 在西沙隆起处计算的异常值与测量的异常值误差较大。在反演过程中也仔细考虑并避免了边界效应。考虑到前人研究发现的西沙隆起广泛分布的断裂后岩浆构造,我们认为剖面L5南端下方还有一个火成岩斜面。岩浆在被动大陆边的断裂和破碎过程中起着关键作用。下地壳高低地壳通常被认为是同步断裂阶段地幔下沉的结果,它在南中国海东北边缘发育达10千米[7, 20, 61]。下地壳HVL的特征是Vp > 7.2 km/s(或Vp > 7.0 km/s)和岩浆成分[10, 20, 62]。因此,HVL 应被视为 2.92-3.05 g/cm3 的高密度体,即下地壳和上地幔的物质混合体[6, 9, 16, 26]。此外,由于岩石圈等静压平衡,地幔上涌会在下地壳产生侧压力[36]。当地幔上升流足够强时,下地壳将被高度拉伸,从而导致高温条件下的下地壳流动[63,64]。最新研究表明,秦岭北麓属于 "岩浆-中间 "型大陆边,具有相当规模的同步岩浆活动[20]。 鉴于上述讨论,我们对整个QDNB的下地壳密度、下地壳厚度、上地幔密度和地壳延伸因子进行了联合解释,以确定地幔下伏的范围。密度反演的多边形可能无法提供准确的高低地壳垂直厚度,其中包括一些主观误差。然而,布格尔重力异常仍然提供了秦岭北麓地下高密度体的信息,可以提供地幔下伏的横向范围。在秦岭北麓大部分地区,特别是地壳延伸系数大于3.00的中部地区,发现了与地幔下伏有关的3.30-3.40 g/cm3的高地幔密度体和2.92-2.96 g/cm3的高地壳下部密度体(图4和图5)。由于埋藏深度较深,在OBS剖面和多道地震剖面中识别岩浆侵入体通常是一项艰巨的任务,需要三维地震数据的清晰图像[19,65]。布格重力异常还为识别大尺度火成岩提供了额外信息,而这些信息在地震剖面解释中可能被忽视。最近的研究表明,移位后的岩浆侵入体可能是同步移位地幔底板的延续[6]。岩浆斜长构造从莫霍面出露,沿西沙海槽轴线侵入极薄的大陆地壳[31]。岩浆侵入体被确定为高密度岩体,底部密度为 3.26 克/立方厘米,顶部密度为 2.64 克/立方厘米。大尺度火成岩只出现在秦岭北麓东部,西沙海槽东端的两个密度为2.94-3.26克/立方厘米的高密度岩体更为明显。在空间上,漂移后岩浆活动由西向东逐渐增强,这也得到了地表热流数据的支持(图1和图5)。最重要的是,2.92-2.96 g/cm3的高低密度地壳岩体和2.64-3.26 g/cm3的岩浆侵入体的识别也得到了以往重力-地震联合反演研究的支持[26,30]。与以往研究的低分辨率相比,我们提出了密度空间变化的细节,并确定了 QDNB 下地幔下沉的范围。岩石圈通常具有流变分层的特征,以脆性变形为主的上地壳通过断裂释放应变,而以塑性变形为主的下地壳则随着温度和深度的增加通过塑性流动释放应变能(图 5(a))[66]。岩浆系统和剥离系统是涉及大陆边缘非均匀断裂的关键过程,似乎在很大程度上控制着岩石圈的流变[11]。突出的剥离断层通常发生在脆性上地壳和韧性下地壳之间或脆性地壳的较浅层位[11]。下地壳底部的岩浆补充可能会使成分、温度和流变学复杂化[48,49]。根据二维稳态热传导方程[67]、Byerlee定律[68]和岩石蠕变定律[69],前人的研究[70]估算了秦岭北麓岩石圈下的流变结构(图5)。在秦岭北麓发现了奶油布丁(CB-1)、果冻夹心-1(JS-1)和果冻夹心-1(JS-2)流变机制,这与密度反演结果和地壳延伸程度有明显的相关性[70](图 5)。CB-1、JS-1 和 JS-2 三种流变机制通常用于描述不同的构造背景。CB-1体系的特点是地壳相对坚固,而上地幔由于活动构造带的高温而明显减弱[71]。JS-1 体系由相对较强、可能是脆性的上地壳和上地幔层组成,被较弱、可能是韧性的下地壳层隔开,下地壳层接近正常大陆地壳[72]。JS-2 机制通常用于描述冷却的大洋岩石圈,它也被称为圣诞树机制,只有一个承重层[49]。QDNB 北部的特点是大陆地壳密度正常,地壳厚度略薄,大于 22 km,地表热流较小,小于 55 mW/m2,扩展因子有限,为 1.25-1。
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Lithosphere
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